对带有分数导数的非线性施罗丁格方程的小振幅单向波的分叉分析
Safoura Rezaei Aderyani1, Reza Saadati2, Mohammad Saeid Abolhassanifar1
1School of Mathematics and Computer Science, Iran University of Science and Technology, Narmak, Tehran, Iran.
Scientific reports
|March 23, 2025
概括
这项研究使用Kudryashov.
科学领域:
- 应用数学 应用数学 应用数学
- 非线性动力学是一种非线性动力学.
- 数学物理学的数学物理.
背景情况:
- 非线性现象在各种科学领域都很普遍.
- 分数计算为复杂系统提供了先进的建模功能.
研究的目的:
- 研究非线性施罗丁格方程和相关模型中的二叉现象.
- 分析分数导数对波浪传播的影响.
- 为了探索修改的本杰明-博纳-马霍尼方程与β导数的行为.
主要方法:
- 应用库德里亚绍夫的方法来得出精确的分析解决方案.
- 分叉分析以了解依赖参数的系统行为.
- 数字模拟和可视化波解.
主要成果:
- 准确的分析解决方案是为非线性时间依赖和分数施罗丁格方程得出的.
- 确定了分数导数对波传播特征的影响.
- 分叉分析揭示了波稳定性和形态学的参数驱动的变化.
结论:
- 该研究成功地应用了分析方法来解决复杂的分数微分方程.
- 这些发现增强了对非线性和分数系统中的波动力学的理解.
- 结果对流体动力学,非线性光学和量子力学有影响.
相关概念视频
Linear Approximation in Frequency Domain
81
Linear systems are characterized by two main properties: superposition and homogeneity. Superposition allows the response to multiple inputs to be the sum of the responses to each individual input. Homogeneity ensures that scaling an input by a scalar results in the response being scaled by the same scalar.
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
In contrast, nonlinear systems do not inherently possess these properties. However, for small deviations around an operating point, a nonlinear system can often be approximated as linear....
81
Linear Approximation in Time Domain
59
Nonlinear systems often require sophisticated approaches for accurate modeling and analysis, with state-space representation being particularly effective. This method is especially useful for systems where variables and parameters vary with time or operating conditions, such as in a simple pendulum or a translational mechanical system with nonlinear springs.
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
59
Velocity and Acceleration of a Wave
3.8K
A wave propagates through a medium with a constant speed, known as a wave velocity. It is different from the speed of the particles of the medium, which is not constant. In addition, the velocity of the medium is perpendicular to the velocity of the wave. The variable speed of the particles of the medium implies that there must be acceleration associated with it.
The velocity of the particles can be obtained by taking the partial derivative of the position equation with respect to time....
The velocity of the particles can be obtained by taking the partial derivative of the position equation with respect to time....
3.8K
Equations of Wave Motion
5.6K
Mathematically, the motion of a wave can be studied using a wavefunction. Consider a string oscillating up and down in simple harmonic motion, having a period T. The wave on the string is sinusoidal and is translated in the positive x-direction as time progresses. Sine is a function of the angle θ, oscillating between +A and −A and repeating every 2π radians. To construct a wave model, the ratio of the angle θ and the position x is considered.
5.6K
Poisson's And Laplace's Equation
2.5K
The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.
2.5K
Traveling Waves: Lossless Lines
114
The provided content explores the behavior of traveling waves on single-phase lossless transmission lines. It begins with a single-phase two-wire lossless transmission line of length Δx, characterized by a loop inductance LH/m and a line-to-line capacitance C F/m. These parameters result in a series inductance LΔx and a shunt capacitance CΔx.
114


